X-Ray Crystallographic Study of Novel Oxazole Derivatives
					
	
		©2016
		Textbook
		
			
				37 Pages
			
		
	
				
				
					
						
					
				
				
				
				
			Summary
			
				This book is the outcome of an examination of Single Organic molecules by Single Crystal X-Ray techniques. The book is suitable for research scholars as it covers a complete analysis of novel Oxazole derivatives by Single Crystal X-Ray techniques.
			
		
	Excerpt
Table Of Contents
Acknowledgements 
First  of  all,  I  would  like  to  thank  Prof.  Anamik  Shah,  *Vice-Chancellor, 
Gujarat  Vidyapith,  Ahmedabad  and  Department  of  Chemistry,  Saurashtra 
University  for  giving  me  an  opportunity  to  carry  out  work  in  his  laboratory 
under  his  guidance.  He  shared  with  me  a  lot  of  his  expertise  and  research 
insight.  His  wide  knowledge  in  the  field  of  Chemistry  research  and  X-Ray 
logical  way  of  thinking  has  been  of  great  value  for  me  to  accomplish  this 
chapter work. I am deeply grateful to the Institute for the trust and support that 
they gave me in order to study in Single Crystal X-Ray Instrumentation, SCX-
mini  model,  Rigaku  Company  at  Center  of  Excellence  (CoE),  National 
Facility  for  Drug  Discovery  Complex,  Department  of  Chemistry,  Saurashtra 
University,  Rajkot,  India.  This book is dedicated to my MOTHER 
"LINABEN RAMANLAL MEHARIYA" on her 50
th
 Birthday.  I  owe  my 
special  thanks  to  my  beloved  wife,  Bhagwati  Krunal  Gauni  Mehariya.  My 
special gratitude is due to  my parents, my sisters and their families for their 
loving  support,  inspiration  to  do  my  best  in  all  matters  of  life.  To  them  I 
dedicate this Chapter. 
This book is also dedicated to my Grand Mother-Valiben 
Mehariya, Maniben Parmar, Mother in Law-Lataben Gauni and 
My Masi-Madhuben Mehariya. 
Krunalkumar Mehariya 
5 
1.  Introduction 
  Oxazole  is  the  aromatic  compound  of  a  wide  range  of  heterocyclic 
aromatic  organic  scaffolds.  Structures  of  Oxazole  mainly  contain  a 
nitrogen atom and an oxygen atom separated by one carbon in a five 
membered ring 
[1]
.  
  Oxazole  is  designated  as  1,  3-oxazoles  to  indicate  the  position  of 
heteroatoms  in  the  ring.  General  structure  of  Oxazole  (1)  is  given 
below. 
Fig. 1 General Structure of Oxazole 
  In the field of hetero cyclic chemistry, Oxazole and its derivatives are 
wide  range  and  consist  of  medicinal  chemistry,  natural  products, 
pharmaceutical chemistry and materials science.  
  Oxazole  heterocyclic  ring  of  the  proton  acidities  have  been 
theoretically calculated and determined experimentally. 
  The acidity of hydrogen atom decreases in the order C(4)C(5) C(2) 
carbon atom. 
  Oxazoles have been found to be common skeleton in several naturally 
isolated compounds and have thus saved attention within the chemical 
and pharmaceutical public
[3-4].
  The characteristic of oxazole skeleton checked by various types of the 
sophisticated analytical techniques. 
  The  IR  spectrum  of  oxazole  shows  absorbance  at  1143,  1080  (ring 
breathing),  1257  (C-H  in  plane  deformation),  1536,  1499,  1327  (ring 
stretch), and1045 cm
-1
. 
  The  UV,  the  
max
  of  Oxazole  depends  highly  on  the  substitution 
pattern.  In  methanol,  the  parent  ring  system  has  an  absorption 
maximum at 
max
 ¼ 205 nm. 
  Oxazole show characteristic resonances in both 
1
H NMR and 
13
C NMR 
spectra. 
  The oxazole compound displays resonances (d) between 7.00 and 8.00 
in the
1
H NMR spectrum, show that the aromatic region present in the 
skeleton, and the presence of substituent can change the chemical shift 
by up to 1 ppm
[4-5].
6 
2.  Oxazole-containing natural products 
  Several  types  of  Oxazole-containing  natural  products  were  isolated 
from various regions and importance in pharmaceuticals as well as in 
synthetic organic fields.  
  A number of oxazole skeletons are present in a great amount of natural 
products  possessing  a  wide  range  of  pharmacological  activities.  The 
past  few  years  of  the  marine  natural  products  with  2,  4-concatenated 
oxazoles have been isolated and synthesized.  
  Indolyl-oxazoles  derivatives  of  5-(indol-3-yl)oxazoles  compounds 
occurs  in  a  variety  of  natural  products  and  possess  a  wide  range  of 
biological importance. 
  A  Pimprinine  (2),  Indolyl-oxazoles  derivatives  has  a  wide  range  of 
biological  activities,  from  antibiotic  and  fungicidal  effects  to 
monoamide oxidase inhibition and anti-epilepsy 
[6].
  Indolyl-oxazoles  derivatives,  Streptochlorin  (3)  has  a  wide-ranging 
fungicidal  activity  and  also  an  anti-proliferative  agent.  Streptochlorin 
has  isolated  from  the  fermentation  broth  of  a  marine  actinomycete 
isolated from marine sediment 
[7].
  A series of the Breitfussins A (4a)and B (4b)are related heterocyclic 
compounds, containing Indolyl-oxazole aromatic ring in the molecules 
and originated from the marine organism Thelia Breitfussi 
[8]
. 
7 
  Breitfussin A and Breitfussin B is core of Indole and Oxazole ring 
with interesting targets in many ways. 
8 
3.  Chemistry 
3.1  Synthesis of 5-(3-methoxy-4-(prop-2-yn-1 yloxy) phenyl) 
oxazole 
3.2  Preparation of 5-(3-methoxy-4-(prop-2-yn-1 yloxy) phenyl) 
oxazole (6) 
The 3-methoxy-4-(prop-2-yn-1-yloxy) benzaldehyde (5) (191 mg, 1.0 mmol), 
TosMIC(196 mg, 1.0 mmol) and K
2
CO
3
 (150 mg, 1.2 mmol) were dissolved 
in methanol (2.0 mL). The solution was stirred at room temperature and reflux 
for  3-4  hours  at  70-75  °C,  until  the  starting  materials  were  not  detected  by 
TLC. Then, the solid formed was filtered and washed with cold water (5 mL) 
used without further purification. 
3.3  Analytical data 
5-(3-methoxy-4-(prop-2-yn-1  yloxy)phenyl)  oxazole(6):  White  solid;  Yield 
90%; mp 180-182 °C; MS: m/z 230. 
9 
4.  X-ray Structure Report 
4.1  Experimental 
4.1.1  Data Collection 
  A  colorless  prism  crystal  of  C
13
H
11
NO
3
  having  approximate 
dimensions  of  0.560  ×  0.480  ×  0.300  mm  was  mounted  on  a  glass 
fiber.  
  All  measurements  were  made  on  a  Rigaku  SCX  mini  diffractometer 
using graphite monochromated Mo-K radiation. 
  The crystal-to-detector distance was 52.00 mm. Cell constants and an 
orientation  matrix  for  data  collection  corresponded  to  a  primitive 
orthorhombic cell with dimensions: a = 17.421(4) Å, b = 18.581(4) Å, 
c = 6.882(2) Å, V = 2227.6(8) Å
3
. 
  For  Z  =  8  and  F.W.  =  229.23,  the calculated  density  is  1.367  g/cm3. 
Based on the reflection conditions of:0kl:  k+l = 2n and h0l:  h = 2n. 
  Packing  considerations,  a  statistical  analysis  of  intensity  distribution, 
and the successful solution and refinement of the structure, the space 
group was determined to be:Pna21 (#33). 
  The data were collected at a temperature of 20 + 1 °C to a maximum 
2 value of 55.0°.  
  A total of 540 oscillation images were collected. A sweep of data was 
done using  oscillations from -120.0 to 60.0° in 1.0° steps.  
  The  exposure  rate  was  10.0  [sec./°].  The  detector  swing  angle  was  -
30.80°.  
  A  second  sweep  was  performed  using    oscillations  from  -120.0  to 
60.0° in 1.0° steps.  
  The exposure rate was 10.0 [sec./°].  
  The detector swing angle was -30.80°.   
  Another  sweep  was  performed  using    oscillations  from  -120.0  to 
60.0° in 1.0° steps.  
  The detector swing angle was -30.80°.  
  The crystal-to-detector distance was 52.00 mm.  
  Readout was performed in the 0.146 mm pixel mode. 
4.1.2  Data Reduction 
  The  20901  reflections  that  were  collected,  5047  were  unique  (R
int
  = 
0.0652), equivalent reflections were merged.  
  Data were collected and processed using CrystalClear (Rigaku). 
  The linear absorption coefficient, , for Mo-K radiation is 0.981 cm
-1
. 
  An  empirical  absorption  correction  was  applied  which  resulted  in 
transmission factors ranging from 0.635 to 0.971. 
  The data were corrected for Lorentz and polarization effects.  
10 
4.1.3  Structure Solution and Refinement 
  The  structure  was  solved  by  direct  methods 
[9]
  and  expanded  using 
Fourier techniques. 
  The non-hydrogen atoms were refined anisotropically. 
  Hydrogen atoms were refined using the riding model. 
  The  final  cycle  of  full-matrix  least-squares  refinement 
[10]
on  F
2
  was 
based  on  5047  observed  reflections  and  319  variable  parameters  and 
converged  (largest  parameter  shift  was  1.19  times  its  esd)  with 
unweighted and weighted agreement factors. 
  The standard deviation of an observation of unit weight 
[11] 
was 0.96. 
  Unit weights were used.   
  The maximum and minimum peaks on the final difference Fourier map 
corresponded to 0.19 and -0.15 e/Å
3
, respectively. 
  The  absolute  structure  was  deduced  based  on  Flack  parameter,  -3(4), 
using 2294 Friedel pairs 
[12].
  Neutral  atom  scattering  factors  were  taken  from  Cromer  and  Waber 
[13]
. 
  Anomalous dispersion effects were included in F
calc
[14]
, the values for 
f' and f were those of Creagh and McAuley 
[15]
.  
  The  values  for  the  mass  attenuation  coefficients  are  those  of  Creagh 
and Hubbell 
[16]
.  
  All  calculations  were  performed  using  the  CrystalStructure 
[17] 
crystallographic  software  package  except  for  refinement,  which  was 
performed using SHELXL-97 
[18-19]
. 
4.2  Experimental Details 
4.2.1  Crystal Data   
Empirical Formula 
C13H11NO3 
Formula Weight 
229.23 
Crystal Color, Habit 
colorless, prism 
Crystal Dimensions 
0.560 ×0.480 × 0.300 mm 
Crystal System 
Orthorhombic 
Lattice Type 
Primitive 
Lattice Parameters 
a =  17.421(4) Å 
b =  18.581(4) Å 
c =   6.882(2) Å 
V = 2227.6(8) Å
3
Space Group 
Pna21 (#33) 
Z value 
8 
D
calc
1.367 g/cm3 
F
000
960.00 
(MoK) 
0.981 cm
-1
11 
4.2.2  Intensity Measurements 
Diffractometer 
SCX mini 
Radiation 
MoK
 ( = 0.71075 Å) 
graphite monochromated 
Voltage, Current 
50kV, 30mA 
Temperature 
20.0oC 
Data Images 
540 exposures 
 oscillation Range  
-120.0 to 60.0° 
Exposure Rate  
10.0 sec./° 
Detector Swing Angle 
-30.80° 
Detector Position 
52.00 mm 
Pixel Size 
0.146 mm 
2
max
55.0° 
No. of Reflections Measured 
Total: 20901 
Unique: 5047 (R
int
 = 0.0652) 
Friedel pairs: 2294 
Corrections 
Lorentz-polarization 
Absorption 
(trans. factors: 0.635 - 0.971) 
4.2.3  Structure Solution and Refinement 
Structure Solution 
Direct Methods (SIR92) 
Refinement 
Full-matrix least-squares on F
2
Function Minimized 
 (F
o
2
 - F
c
2
)
2 
Least Squares Weights 
 = 1/ [ 
2
(F
o
2
) + (0.0455 . P)
2
+ 1.0896 .P] 
where P = (Max(F
o
2
0) + 2F
c
2
)/3 
2 max cutoff 
55.0° 
Anomalous Dispersion 
All non-hydrogen atoms 
No. Observations (All 
reflections) 
5047 
No. Variables 
319 
Reflection/Parameter Ratio 
15.82 
Residuals: R
1
 (I2.00(I)) 
0.0538 
Residuals: R (All reflections) 
0.0947 
Residuals: wR2 (All 
reflections) 
0.1404 
Goodness of Fit Indicator 
0.961 
Flack Parameter 
(Friedel pairs = 2294) 
-3(4) 
Max Shift/Error in Final Cycle  1.185 
Maximum peak in Final Diff. 
Map 
0.19 e /Å
3
Minimum  peak  in  Final  Diff. 
Map 
-0.15 e /Å
3
Details
- Pages
- Type of Edition
- Erstausgabe
- Publication Year
- 2016
- ISBN (Softcover)
- 9783960670834
- ISBN (PDF)
- 9783960675839
- File size
- 3.9 MB
- Language
- English
- Publication date
- 2016 (September)
- Keywords
- X-ray Structure Report Oxazole Single Crystal X-Ray Instrumentation Hetero cyclic chemistry Molecular chemistry
- Product Safety
- Anchor Academic Publishing
 
					